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10.5 Long-Memory Models 361<br />

and<br />

Cov(Y (t + h), Y (t)) b ′ e Ah b.<br />

Inference for continuous-time ARMA processes is more complicated than for<br />

continuous-time AR(1) processes because higher-order processes are not Markovian,<br />

so the simple calculation that led to (10.4.6) must be modified. However, the<br />

likelihood of observations at times t1,...,tn can still easily be computed using the<br />

discrete-time Kalman recursions (see Jones, 1980).<br />

Continuous-time ARMA processes with thresholds constitute a useful class of<br />

nonlinear time series models. For example, the continuous-time threshold AR(1)<br />

process with threshold at r is defined as a solution of the stochastic differential<br />

equations<br />

and<br />

10.5 Long-Memory Models<br />

dX(t) + a1X(t)dt b1 dt + σ1dB(t), X(t) ≤ r,<br />

dX(t) + a2X(t)dt b2 dt + σ2dB(t), X(t) > r.<br />

For a detailed discussion of such processes, see Stramer, Brockwell, and Tweedie<br />

(1996). Continuous-time threshold ARMA processes are discussed in Brockwell<br />

(1994) and non-Gaussian CARMA(p, q) processes in Brockwell (2001). For more<br />

on continuous-time models see Bergstrom (1990) and Harvey (1990).<br />

The autocorrelation function ρ(·) of an ARMA process at lag h converges rapidly to<br />

zero as h →∞in the sense that there exists r>1 such that<br />

r h ρ(h) → 0 as h →∞. (10.5.1)<br />

Stationary processes with much more slowly decreasing autocorrelation function,<br />

known as fractionally integrated ARMA processes, or more precisely as ARIMA<br />

(p, d, q) processes with 0 < |d| < 0.5, satisfy difference equations of the form<br />

(1 − B) d φ(B)Xt θ(B)Zt, (10.5.2)<br />

where φ(z) and θ(z) are polynomials of degrees p and q, respectively, satisfying<br />

φ(z) 0 and θ(z) 0 for all z such that |z| ≤1,<br />

B is the backward shift operator, and {Zt} is a white noise sequence with mean 0 and<br />

variance σ 2 . The operator (1 − B) d is defined by the binomial expansion<br />

(1 − B) d ∞<br />

πjB j ,<br />

j0

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